Discrete spectrum asymptotics for the three-particle Hamiltonians on lattices

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dc.creatorAlbeverio, Sergio
dc.creatorLakaev, Saidakhmat N.
dc.creatorXalxo'jaev, Axmad M.
dc.date2007-03-11
dc.date.accessioned2026-07-07T07:51:25Z
dc.date.available2026-07-07T07:51:25Z
dc.descriptionWe consider the Hamiltonian of a system of three quantum mechanical particles on the three-dimensional lattice $\Z^3$ interacting via short-range pair potentials. We prove for the two-particle energy operator $h(k),$ $k\in \T^3$ the two-particle quasi-momentum, the existence of a unique positive eigenvalue $z(k)$ lying below the essential spectrum under assumption that the operator $h(0)$ corresponding to the zero value of $k$ has a zero energy resonance. We describe the location of the essential spectrum of the three-particle discrete Schrödinger operators $H(K)$,$K$ the three-particle quasi-momentum by the spectra of $h(k), k\in \T^3.$ We prove the existence of infinitely many eigenvalues of H(0) and establish for the number of eigenvalues $N(0,z)$ lying below $z<0$ the asymptotics \begin{equation*}\label{asimz} \lim\limits_{z \to -0}\frac{N(0,z)}{|\log |z||}=\frac{λ_0}{2π}, \end{equation*} where $λ_0$ a unique positive solution of the equation $$ λ= \frac{8 \sinh πλ/6}{\sqrt 3 \cosh πλ/2}.$$ We prove that for all $ K \in U_δ^0(0),$ where $U_δ^0(0)$ some punctured $δ>0$ neighborhood of the origin, the number $N(K,0)$ of eigenvalues the operator $H(K)$ below zero is finite and satisfy the asymptotics \begin{equation*}\label{asimk} \lim\limits_{|K| \to 0}\frac{N(K,0)}{|\log |K||}=\frac{λ_0}π. \end{equation*}
dc.description25 pages
dc.identifierhttps://arxiv.org/abs/math/0703301
dc.identifierhttp://arxiv.org/abs/math/0703301
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/125504
dc.subjectSpectral Theory
dc.subjectPrimary: 81Q10, Secondary: 35P20, 47N50
dc.titleDiscrete spectrum asymptotics for the three-particle Hamiltonians on lattices
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